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Three \(9.0-\Omega\) resistors are connected in series with a \(12-\mathrm{V}\) battery. Find (a) the equivalent resistance of the circuit and (b) the current in each resistor. (c) Repeat for the case in which all three resistors are connected in parallel across the battery,

Short Answer

Expert verified
For the series circuit, the equivalent resistance is \(27.0 - \Omega\) and the current is \(0.44 - A\). For the parallel circuit, the equivalent resistance is \(3.0-\Omega\) and the current in each resistor is \(1.33 - A\).

Step by step solution

01

Equivalent Resistance for Series Circuit

3 resistors each of \(9.0 - \Omega\) are in series, so their equivalent is calculated as \(R_{eq} = R_1 + R_2 + R_3 = 9.0\Omega + 9.0\Omega + 9.0\Omega = 27.0\Omega\)
02

Current in Series Circuit

Applying Ohm's Law, which is \(I = V / R\), the current in the circuit is calculated as \(I = 12V / 27.0\Omega = 0.44A\). Therefore, the current in each resistor is also 0.44 A, because in a series circuit, the current is the same in all parts of the circuit.
03

Equivalent Resistance for Parallel Circuit

Same resistors are now in a parallel circuit. The equivalent is calculated as \(1 / R_{eq} = 1 / 9.0\Omega + 1 / 9.0\Omega + 1 / 9.0\Omega = 1 / 3.0\Omega\). Therefore, \(R_{eq} = 3.0\Omega\).
04

Current in Parallel Circuit

Applying Ohm's Law, the total current in the circuit is \(I = V / R = 12V / 3.0\Omega = 4.0A\). In a parallel circuit, the voltage is the same across all paths, therefore the current in each resistor will be \(I = V / R = 12V / 9.0\Omega = 1.33A\).

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Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Ohm's Law
Understanding Ohm's Law is fundamental to grasping the concepts of both series and parallel circuits. Ohm's Law states that the current flowing through a conductor between two points is directly proportional to the voltage across the two points and is given by the formula:
  • \( I = \frac{V}{R} \)
Here, \( I \) is the current in amperes (A), \( V \) is the voltage in volts (V), and \( R \) is the resistance in ohms (\( \Omega \)).
In our example, when you connect a battery with a voltage of 12 volts to a circuit, you can determine how much current flows through resistors by using this relationship.
Ohm's Law is crucial as it helps us understand the behavior of electrical components when they are connected to a power source. By applying it to both series and parallel circuits, we can calculate the current and verify how resistances affect the circuit's operation.
Series Circuit
In a series circuit, resistors are connected one after another, forming a single pathway for the electric current.
This means that the same current flows through each resistor.
The total or equivalent resistance \( R_{eq} \) of resistors in a series circuit is simply the sum of their individual resistances:
  • \( R_{eq} = R_1 + R_2 + R_3 + ... \)
For our given problem, with three resistors each being 9.0 ohms, the equivalent resistance is calculated as \( 27.0 \Omega \).
This greater resistance means that the current flowing through the series circuit will be less, due to the greater opposition posed by all the resistors combined.
Using Ohm's Law, the current can be calculated as \( I = \frac{V}{R} = \frac{12V}{27.0\Omega} = 0.44A \).
Each resistor will have the same current of 0.44 Amps, which is a typical characteristic of series circuits.
Parallel Circuit
A parallel circuit has multiple paths for the electricity to flow, as each resistor is connected across the same two points. In such arrangements:
  • The voltage across each resistor is the same, equal to the battery's voltage.
  • The current may vary through each path, depending on the resistance in that path.
To find the equivalent resistance \( R_{eq} \) in a parallel circuit, we use the formula:
  • \( \frac{1}{R_{eq}} = \frac{1}{R_1} + \frac{1}{R_2} + \frac{1}{R_3} + ... \)
For the given resistors, this results in \( R_{eq} = 3.0 \Omega \).
This lower equivalent resistance increases the total current in the circuit.
Using Ohm's Law, you calculate the total current as \( I = \frac{V}{R} = \frac{12V}{3.0\Omega} = 4.0A \).
Each resistor has the same voltage of 12V, and the current through each resistor can be found using \( I = \frac{V}{R} = \frac{12V}{9.0\Omega} = 1.33A \).
Hence, in a parallel circuit, while the voltage remains the same across all resistors, the current is divided among the paths.

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Most popular questions from this chapter

A voltage \(\Delta V\) is applied to a series configuration of \(n\) resistors, each of resistance \(R\). The circuit components are reconnected in a parallel configuration, and voltage \(\Delta V\) is again applied. Show that the power consumed by the series configuration is \(1 / n^{2}\) times the power consumed by the parallel configuration.

The student engineer of a campus radio station wishes to verify the effectiveness of the lightning rod on the antenna mast (Fig. P18.55, page 624). The unknown resistance \(R_{x}\) is between points \(C\) and \(E\). Point \(E\) is a "true ground," but is inaccessible for direct measurement because the stratum in which it is located is several meters below Earth's surface. Two identical rods are driven into the ground at \(A\) and \(B\), introducing an unknown resistance \(R_{y}\). The procedure for finding the unknown resistance \(R_{x}\) is as follows. Measure resistance \(R_{1}\) between points \(A\) and \(B\). Then connect \(A\) and \(B\) with a heavy conducting wire and measure resistance \(R_{2}\) between points \(A\) and \(C\). (a) Derive a formula for \(R_{x}\) in terms of the observable resistances \(R_{1}\) and \(R_{2}\). (b) A satisfactory ground resistance would be \(R_{x}<2.0 \Omega\). Is the grounding of the station adequate if measurements give \(R_{1}=13 \Omega\) and \(R_{2}=6.0 \Omega ?\)

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An emf of \(10 \mathrm{~V}\) is connected to a series \(R C\) circuit consisting of a resistor of \(2.0 \times 10^{6} \Omega\) and a capacitor of \(3.0 \mu \mathrm{F}\). Find the time required for the charge on the capacitor to reach \(90 \%\) of its final value.

Show that \(\tau=R C\) has units of time.

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